真空电弧和气体电弧在阈值电流下的腐蚀速率

A. Murzakaev
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摘要

本文报道了在真空中脉冲电弧在表面条件(污染物和清洁)和环境气体(氩气、压力为600托的高纯度氮气)和冷阴极影响下的侵蚀速率实验研究。研究了电弧前加热温度低于熔化温度制备的Au, Ag, Cu, W线阴极的腐蚀速率。这样的表面可以足够干净,也没有事先的侵蚀。在这两种系统中,离子流都是用偏压收集器测量的。看来侵蚀速率不受外部背景气体的影响。离子收集和称重方法之间的差异清楚地指出了大颗粒对阴极侵蚀的贡献。研究表明,宏观粒子的质量损失确实很重要。实验结果表明,大颗粒通量去除的正极材料的质量大于以离子形式留下的正极材料的质量。此外,还采用称重法测定了阴极材料的总腐蚀速率。通过对真空电弧和气体中电弧的电荷转移速率与侵蚀速率的关系分析,得出电弧转移的电荷较小时,总侵蚀速率接近离子侵蚀速率。离子电流与真空电弧电流呈线性关系。电弧电流的近似独立性与增加电弧电流导致发射中心数量增加而不是改变这些中心的特征的发现是一致的。
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Erosion rate in a vacuum arc and in a gas arc at threshold currents
The present paper reports an experimental study of the erosion rate of pulsed arcs in vacuum under the influence of surface conditions (contaminants and clean), and ambient gases (argon, nitrogen with high purity introduced with pressures 600 Torr) with cold cathodes. Erosion rates have been studied of wires cathodes from Au, Ag, Cu, W prepared by heating less then melting temperature prior to arcing. Such surfaces may be sufficiently clean also without preceding erosion. In both systems the ion current streaming was measured by a biased collector. It appears that the erosion rates are not changed by outer influences background gas. The discrepancy between the ion collection and weighing methods clearly points to the contribution of macroparticles to cathode erosion. It has been shown that macroparticle mass losses are indeed important. Experimental results show that the mass of cathode material removed by the macroparticles flux is greater than the mass of cathode material leaving in form of ions. Besides ion current measurements also used the weighing method to determine the total erosion rate of cathode materials. From the analysis of the erosion rate as a function of charge transferred by the vacuum arc and arc in gases were concluded that the total erosion rate approaches the ion erosion rate if the charge transferred by the arc is small. The dependence of the ion current from vacuum arc current is in linear relation. The approximate independence of arc current is consistent with findings that increasing the arc current leads to an increase in the number of emission centers rather than changing the character of these centers.
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